Photodiode having quantum dot light absorption layer

ABSTRACT

A photodiode comprising a photoactive spinel oxide layer is described. This photoactive spinel oxide layer forms a contact with both a light absorption layer of quantum dots, quantum wires, or quantum rods, and an inorganic substrate layer. In some embodiments, the inorganic substrate layer and the photoactive spinel oxide layer form an isotype junction. Methods of characterizing the photodiode are provided and demonstrate commercially relevant electrical and optoelectronic properties, particularly the ability to operate as a photodetector with a high photosensitivity. An economical process for preparing the photodiode is provided as well as applications.

CROSS-REFERENCE TO RELATED APPLICATIONS

The present application is a Continuation of Ser. No. 15/492,267, nowallowed, having a tiling date of Apr. 20, 2017.

BACKGROUND OF THE INVENTION Technical Field

The present invention relates to a photodiode comprising a spinel oxidelayered between a light absorption layer and an inorganic semiconductor.

Description of the Related Art

The “background” description provided herein is for the purpose ofgenerally presenting the context of the disclosure. Work of thepresently named inventors, to the extent it is described in thisbackground section, as well as aspects of the description which may nototherwise qualify as prior art at the time of filing, are neitherexpressly or impliedly admitted as prior art against the presentinvention.

Optoelectronic devices generate electric current from electromagneticradiation. For example, optoelectronic devices can convert solar lightinto electric current. Optoelectronic devices may include photosensitivedevices. Optoelectronic devices may also generate electric current fromother various light sources. Another type of optoelectronic device is aphotodiode, which may detect an electric signal caused by sunlightabsorption. In operation, a photodiode with a heterojunction structureis used to detect the electric current, or photocurrent. Photodiodes maybe further characterized by their rectifying properties under differentexternally applied voltages and light intensities. Conventionaloptoelectronic devices may be manufactured from inorganic semiconductorssuch as silicon, gallium arsenide, indium phosphide and others, whichalso function as the photoactive layer. The photoactive layer may bechosen for certain absorption properties to effectively generateelectric current via different types of electromagnetic radiation.

A functional material is described below for the photoactive layer in aphotodiode. A photodiode includes a photoactive layer, metal electrodes,and an encapsulation. The photoactive layer absorbs the light andconverts the light energy to current or voltage.

The light can be absorbed when the light energy is greater than the bandgap value of the semiconductor and an exciton is formed. In this lightabsorbing process, a charge separation occurs and photoconductive andphotovoltaic effects take place in the photodiode.

Photodiodes are typically formed by various combinations ofsemiconductors such as p-type (hole conducting) semiconductors or n-type(free electron conducting) semiconductors. When two n-typesemiconductors or two p-type semiconductors are used in the same deviceto form a p-p junction or an n-n junction, this device is known as anisotype photodiode. There is a need for such isotype photodiodes,especially with high performance parameters, low material costs, andreliable fabrication methods. There is also need for a photodiode thatcan be adjusted to different solar light sensitivities.

In view of the foregoing, one objective of the present invention is toprovide a photodiode comprising a photoactive spinel oxide layeredbetween a light absorption layer and an inorganic semiconductor. In oneaspect of the invention the photodiode further comprises an isotypejunction.

BRIEF SUMMARY OF THE INVENTION

According to a first aspect, the present disclosure relates to aphotodiode comprising an ohmic contact having a first work function, aninorganic substrate layer in continuous contact with the ohmic contact,a photoactive layer in continuous contact with the inorganic substratelayer, a light absorption layer in continuous contact with thephotoactive layer, and a top electrode in contact with the lightabsorption layer, where the top electrode has a second work function.The inorganic substrate layer of the photodiode comprises asemiconductor. The photoactive layer comprises a spinel metal oxide of ageneral formula A²⁺(B³⁺)₂(O²⁻)₄ where A and B are metal ions. The lightabsorption layer of the photodiode comprises at least one materialselected from the group consisting of quantum dots, quantum rods, andquantum wires. Also, the second work function of the top electrode isgreater than the first work function of the ohmic contact.

In one embodiment of the photodiode, the light absorption layercomprises quantum dots of at least one material selected from the groupconsisting of lead sulfide (PbS), lead selenide (PbSe), lead telluride(PbTe), cadmium selenide (CdSe), cadmium sulfide (CdS), and cadmiumtelluride (CdTe).

In one embodiment of the photodiode, the metal ion A is at least oneselected from the group consisting of Zn, Cu, Co, Mn, Ni, Mg, Be, andTi, and the metal ion B is at least one selected from the groupconsisting of Al, Fe, Cr, and V.

In one embodiment of the photodiode, the photoactive layer comprises aspinel metal oxide selected from the group consisting of ZnFe₂O₄,CuFe₂O₄, CoFe₂O₄, MnFe₂O₄, and NiFe₂O₄.

In one embodiment of the photodiode, the spinel metal oxide has a directoptical band gap of 2.0-3.0 eV.

In one embodiment of the photodiode, the semiconductor of the inorganicsubstrate layer comprises at least one selected from the groupconsisting of silicon, germanium, indium gallium arsenide, lead (II)sulfide, indium phosphor, and mercury cadmium telluride.

In one embodiment of the photodiode, the semiconductor of the inorganicsubstrate layer is a p-type silicon based semiconductor.

In one embodiment of the photodiode, the optical band gap of thephotoactive layer is greater than the optical band gap of the lightabsorption layer.

In one embodiment of the photodiode, the inorganic substrate layer has athickness of 200-600 μm.

In one embodiment of the photodiode, the photoactive layer has athickness of 20-250 nm.

In one embodiment of the photodiode, the light absorption layer has athickness of 10-100 nm.

In one embodiment of the photodiode, the inorganic substrate layer andthe photoactive layer form an isotype junction.

In one embodiment of the photodiode, the top electrode is aluminum.

In one embodiment of the photodiode, the inorganic substrate layer has aresistivity of 1-10 Ω·cm.

In one embodiment, the photodiode has a barrier height of 0.5-1.25 eV.

In one embodiment, the photodiode has a photoresponsivity of 0.10-0.40A/W.

In one embodiment, the photodiode has a photosensitivity defined as theratio of illuminated current to dark current of 6000-7500 at a bias of5.0-8.0 V.

According to a second aspect, the present disclosure relates to a methodfor forming the photodiode of the first aspect. These steps involvedepositing the ohmic contact onto the inorganic substrate layer; spin ordrop coating the spinel metal oxide onto the inorganic substrate layer,to form the photoactive layer; spin or drop coating quantum dots,quantum rods, or quantum wires onto the photoactive layer, therebyforming the light absorption layer; and depositing the top electrodeonto the light absorption layer.

According to a third aspect, the present disclosure relates to a methodof generating an electronic current using the photodiode of the firstaspect. This method involves irradiating the photodiode of the firstaspect with a light source having a wavelength of 150-1500 nm.

According to a fourth aspect, the present disclosure relates to anelectronic device comprising the photodiode of the first aspect.

The foregoing paragraphs have been provided by way of generalintroduction, and are not intended to limit the scope of the followingclaims. The described embodiments, together with further advantages,will be best understood by reference to the following detaileddescription taken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

A more complete appreciation of the disclosure and many of the attendantadvantages thereof will be readily obtained as the same becomes betterunderstood by reference to the following detailed description whenconsidered in connection with the accompanying drawings, wherein:

FIG. 1 shows an example of a method for forming a photodiode.

FIG. 2 is a diagram of the structure of a photodiode.

FIG. 3A is a scanning electron microscopy (SEM) image of ZnFe₂O₄ spineloxide nanorods.

FIG. 3B is an electron diffraction spectroscopy (EDS) measurement ofZnFe₂O₄ spinel oxide nanorods.

FIG. 4 is a plot of the current of a photodiode at different biasvoltages and at different illumination intensities.

FIG. 5 is a plot of a photodiode's photoresponsivity at different biasvoltages and with an illumination intensity of 100 mW/cm².

FIG. 6 is a plot of a photodiode's photosensitivity at different biasvoltages and with an illumination intensity of 100 mW/cm².

DETAILED DESCRIPTION OF THE EMBODIMENTS

The present disclosure will be better understood with reference to thefollowing definitions. As used herein, the words “a” and “an” and thelike carry the meaning of “one or more.” Within the description of thisdisclosure, where a numerical limit or range is stated, the endpointsare included unless stated otherwise. Also, all values and subrangeswithin a numerical limit or range are specifically included as ifexplicitly written out.

As used herein, “electric current” refers to a rate of flow of electriccharge. Loosely-bound electrons are considered as free electrons,capable of moving throughout the material, and considered the negativecharge carriers. An electron hole is the absence of an electron from avalence band and allows conceptualization of interactions betweenelectrons and a nearly full system. The electron holes are the positivecharge carriers in materials missing a valence electron, for example,certain semiconductor crystals.

As used herein, the term “transparent” refers to a property of amaterial that allows an average transmission of at least 80% of anincident electromagnetic radiation having a wavelength in a range fromabout 150 nm to about 1500 nm.

In classical semiconductors, electrons may have energies only withincertain ranges of energy levels, termed bands. These bands are locatedenergetically between the ground state energy (the energy of electronstightly bound to the atomic nuclei of the material) and the freeelectron energy (the energy required for an electron to escape entirelyfrom the material). The majority of low energy states, close to thenucleus, are occupied by electrons up to a particular band energy levelcalled the valence band. In metals and conductors, the valence band istypically filled with electrons, so extra electrons occupy a conductionband, which is an energy level immediately above the valence band.Semiconductors and insulators, in contrast, have very few(semiconductor) or virtually none (insulator) of their electronsavailable in the conduction band.

The ease with which electrons in a semiconductor material can be excitedfrom the valence band to the conduction band depends upon the band gap,which is the energy difference between the two bands. The size of thisenergy band gap serves as a functional difference between semiconductorsand insulators.

A semiconductor has an electrical conductivity of 10⁻²-10⁴ S/cm, whichis intermediate in magnitude between that of a conductor and insulator.In a semiconductor it may be more useful to think of the current as dueto the flow of positive “holes.” The current which flows in an intrinsicsemiconductor consists of both electron and hole current. Electronswhich have been freed from their lattice positions into the conductionband can move through the material. Additionally, electrons can jumpbetween lattice positions to fill the vacancies left by the freedelectrons. This additional mechanism is called hole conduction, andworks as if the holes are migrating across the material in a directionopposite to the free electron movement.

In a semiconductor at a temperature above absolute zero, some electronsmay produce a small current by being excited across the band gap andinto the conduction band. These electrons crossing the gap each leavebehind an electron vacancy or hole. Under the influence of an externalvoltage, both the electron and the hole can move across the material. Inan n-type semiconductor, the dopant contributes extra electrons, whichdramatically increases its conductivity. In a p-type semiconductor thedopant produces extra vacancies or holes, which likewise increases theconductivity. The behavior of a semiconductor junction is the key to avariety of solid-state electronic devices and will be discussed herein.

A material's band structure may be further described by the Fermi level,which is the hypothetical energy level that has a 50% probability ofbeing occupied by an electron at any given time at thermal equilibrium.In doped semiconductors, p-type and n-type, the Fermi level lies in theband gap, in a position that is shifted to lower or higher energies bythe type and amount of doping.

N-type semiconductors have a larger electron concentration than holeconcentration. The phrase “n-type” describes the negative charge of theelectron. In n-type semiconductors, electrons are the majority carriers,and holes are the minority carriers. N-type semiconductors are createdby doping an intrinsic semiconductor with donor impurities. A commondopant for n-type silicon is phosphorus. In an n-type semiconductor, theFermi level is greater than that of the intrinsic (undoped)semiconductor and lies closer to the conduction band than the valenceband.

P-type semiconductors have a larger hole concentration than electronconcentration. The phrase “p-type” describes the positive charge of thehole. In p-type semiconductors, holes are the majority carriers, andelectrons are the minority carriers. P-type semiconductors are createdby doping an intrinsic semiconductor with acceptor impurities. A commonp-type dopant for silicon is boron. For p-type semiconductors, the Fermilevel is below the intrinsic Fermi level and lies closer to the valenceband than the conduction band.

Photocurrent is the electrical current through a photosensitive device,such as a photodiode, as the result of exposure to electromagneticradiation. The photocurrent may be caused by the photoelectric or thephotovoltaic effect. In the photovoltaic effect, when solar light or anyother light is incident upon a material surface, the electrons presentin the valence band absorb energy and, being excited, transition to theconduction band as unbound electrons. These highly excited, non-thermalelectrons diffuse, and some reach a junction where they are acceleratedinto a different material by a built-in potential. This generates anelectromotive force, and thus some of the light energy is converted intoelectric energy. In contrast, the photoelectric (or photoemissive)effect is when electrons are ejected from a material's surface into avacuum upon exposure to light. When the ejected electron is captured byanother electrode, some electric energy is generated. The photovoltaiceffect differs as the excited electrons pass directly from one materialto another, rather than passing through a vacuum.

As used herein, a photodiode is a semiconductor device that convertslight into current. A current may be generated when photons are absorbedby the photodiode. A small amount of current, termed dark current, mayalso be produced when the photodiode is under a forward or reverse biasvoltage with no light present.

According to a first aspect, the present disclosure relates to aphotodiode comprising an ohmic contact 24 having a first work function,an inorganic substrate layer 26 in continuous contact with the ohmiccontact 24, a photoactive layer 28 in continuous contact with theinorganic substrate layer 26, a light absorption layer 30 in continuouscontact with the photoactive layer 28, and a top electrode 32 in contactwith the light absorption layer 30, where the top electrode 32 has asecond work function. The inorganic substrate layer 26 of the photodiodecomprises a semiconductor. The photoactive layer 28 comprises a spinelmetal oxide of a general formula A²⁺(B³⁺)₂(O²⁻)₄ where A and B are metalions. The light absorption layer 30 of the photodiode comprises at leastone material selected from the group consisting of quantum dots, quantumrods, and quantum wires. Also, the second work function of the topelectrode 32 is greater than the first work function of the ohmiccontact 24. Preferably the layers of the photodiode occupy parallelplanes, though in an alternative embodiment, the layers may comprisecurved surfaces.

The ohmic contact 24 may be considered a “bottom electrode,” and maycomprise copper, gold, silver, aluminum, nickel, indium, gallium,tungsten, molybdenum, palladium, titanium, cobalt, and/or platinum witha layer thickness of 50 nm-5 μm, preferably 75 nm -1 μm, more preferably100 nm-500 nm. Alternatively, the ohmic contact 24 may comprise adifferent metal or a metal alloy having an electrical resistivity of atmost 10⁻⁶ Ω·m, preferably at most 10⁻⁷ Ω·m at 20° C.

One side of the ohmic contact 24 is in continuous contact with theinorganic substrate layer 26, though in an alternative embodiment, theohmic contact 24 may be applied as a pattern to the inorganic substratelayer 26, leaving exposed regions. The inorganic substrate layer 26comprises a semiconductor. In one embodiment, the inorganic substratelayer 26 may contain more than 70 wt %, preferably more than 80 wt %,preferably more than 90 wt % semiconductor, and in a preferredembodiment, the inorganic substrate layer 26 is 100 wt %, or completelya semiconductor. Where the inorganic substrate layer 26 is less than 100wt % semiconductor, the composition may also comprise an organicsemiconductor matrix such as polyvinylcarbazole (PVK),poly(3-hexylthiophene) (P3HT), PBBDTTT-CT, phthalocyanine complex, aporphyrin complex, a polythiophene (PT), a derivative of polythiophene,a polycarbazole, a derivative of polycarbazole, a poly(p-phenylenevinylene) (PPV), a PPV derivative, a polyfulorene (PF), abenzodithiophene (BDT)-based polymer, a PF derivative, acyclopentadithiophene-based polymer, a P3DOT, P30T, PMeT, P3DDT, PDDTV,PQT, F8T2, PBTTT-C12, PFDDTBT, BisEH-PFDTBT, BisDMO-PFDTBT, PCDTBT orcombinations and mixtures thereof. In one embodiment, the semiconductorcomprises silicon, germanium, indium gallium arsenide, lead (II)sulfide, indium phosphor, and/or mercury cadmium telluride. In otherembodiments, the semiconductor may be a group IV semiconductor, such assilicon or germanium, and may be doped with aluminum, boron,phosphorous, or gallium. Alternatively, the semiconductor may be a groupIII-V semiconductor such as aluminum phosphide, aluminum arsenide,gallium arsenide, or gallium nitride and doped with beryllium, zinc,cadmium, silicon, or germanium. In a preferred embodiment, thesemiconductor is a p-type silicon based semiconductor, such as silicondoped with boron gallium, aluminum, nitrogen, or indium. However, in ananother embodiment, the semiconductor may be an n-type semiconductorsuch as silicone doped with phosphorus, arsenic, antimony, bismuth, orlithium, or the semiconductor may be a non-silicon p-type semiconductor.In one embodiment, the inorganic substrate layer 26 has a layerthickness of 200-600 μm, preferably 300-500 μm, more preferably 350-450μm. However, in other embodiments, the inorganic substrate layer 26 mayhave a thickness of less than 200 μm or greater than 600 μm. In oneembodiment, the inorganic substrate layer 26 has a resistivity of 1-10Ω·cm, preferably 2-9 Ω·cm, more preferably 3-8 Ω·cm.

A side of the inorganic substrate layer 26 not in contact with the ohmiccontact 24 is in contact with the photoactive layer 28, and thephotoactive layer 28 may have a thickness of 20-250 nm, preferably30-200 nm, more preferably 50-100 nm. The photoactive layer 28 comprisesa spinel metal oxide and may also be known as a “spinel oxidesemiconductor layer.” As defined here, a spinel metal oxide is a metaloxide with the formula A²⁺(B³⁺)₂(O²⁻)₄ where “A” and “B” are metal ions.In one embodiment, “A” may be Zn, Cu, Co, Mn, Ni, Mg, Be, and/or Ti,while “B” may be Al, Fe, Cr, and/or V. In a preferred embodiment, “B” isFe. In one embodiment, the spinel metal oxide has a direct optical bandgap of 2.0-3.0 eV, preferably 2.1-2.9 eV, more preferably 2.2-2.8 eV.Preferably the spinel metal oxide is in the form of a crystal, with theoxide anions arranged in a cubic close-packed lattice, and with themetal ions occupying octahedral and/or tetrahedral sites within thelattice. Preferably the A²⁺ metal ions occupy the tetrahedral sites, andthe B³⁺ metal ions occupy the octahedral sites, though there may beinstances where the metal ions are switched. The A²⁺ and B³⁺ metal ionsmay occupy sites in the lattice at regular spacings or may bedistributed randomly. In one embodiment, the spinel oxide may be in theform of different nanostructured materials, including, but not limitedto nanowires, nanorods, tetrapods, nanobelts, nanoflowers,nanoparticles, nanoflakes, nanosheets, nanospheres, nanoreefs,nanotubes, nanocylinders, nanoboxes, and/or nanostars. In a preferredembodiment, the spinel oxide may be in the form of nanorods ornanowires. For instance, FIG. 3A shows an SEM image of a ZnFe₂O₄ spineloxide in the form of nanowires having widths of 35-45 nm and lengths ofabout 170-350 nm, and FIG. 3B shows an electron diffraction spectrummeasurement. Different nanostructures and compositions of spinel metaloxides may have different optical properties, for instance, differentdirect optical band gaps.

In one embodiment, the spinel metal oxide is ZnFe₂O₄, CuFe₂O₄, CoFe₂O₄,MnFe₂O₄, and/or NiFe₂O₄, and in a preferred embodiment, the spinel metaloxide is ZnFe₂O₄. In other embodiments, the spinel metal oxide may beMgAl₂O₄, BeAl₂O₄, ZnAl₂O₄, FeAl₂O₄, MnAl₂O₄, MgFe₂O₄, (Fe²⁺)(Fe³⁺)₂O₄,TiFe₂O₄, FeCr₂O₄, MgCr₂O₄, ZnCr₂O₄, FeV₂O₄, or MgV₂O₄. In someembodiments, the spinel oxide may comprise a mixture of different metalions with the same charge, for example, (Mg_(x)Fe_(1-x))Al₂O₄ where “x”is between 0 and 1 exclusive. Different metal ions having the samecharge may be distributed at regular spacings throughout the crystallattice tetrahedral and octahedral sites, or may be randomlydistributed. In alternative embodiments, other metal oxides havingsimilar structures may be used despite not being spinel metal oxides.For example, these metal oxides may be (Mg,Fe)₂SiO₄, BeMgAl₄O₈, or(Mg,Fe,Zn)₂BeAl₆O₁₂. In another embodiment, the spinel metal oxide maybe doped with 0.5-2 wt % of a doping agent to change an electronicproperty, for instance, by introducing electron holes or valenceelectrons, similar to doping a silicon-based semiconductor. The dopingagents may include silicon, phosphorous, boron, alkaline-earth metals(such as Ca, Ba, or Sr), alkali metals (such as Na, K, Li), gallium,germanium, arsenic, indium, antimony, bismuth, or lead. In oneembodiment, the photoactive layer 28 may comprise 100 wt % spinel metaloxide. In another embodiment, the photoactive layer 28 may comprise70-99 wt %, 80-98 wt %, or 85-95 wt % spinel metal oxide within asemiconductor matrix. The semiconductor matrix may be an inorganicsemiconductor or organic semiconductor material as mentioned previously.The semiconductor matrix on its own may have a band gap energy higher orlower than the band gap energy of the spinel metal oxide on its own. Inanother embodiment, the semiconductor matrix may have a similar band gapenergy but may be present to modify other electronic or opticalproperties of the photoactive layer 28. Likewise, a matrix material maybe used to support the structure or dispersion of the spinel metaloxide, and this matrix material may not significantly contribute orchange the optical properties of the photoactive layer 28. In oneembodiment, the matrix material may be a polymer matrix ofpolymethylmethacrylate (PMMA), polystyrene, polyimides, or some otherpolymer to encapsulate a nanostructured spinel oxide and restrict themovement of individual particles or structures. In one embodiment, ananostructured spinel metal oxide may be on the inorganic substratelayer 26 without a matrix and comprise 70-95 vol %, or 80-90 vol % ofthe photoactive layer 28, with the remaining volume comprising air or aninert gas, such as Ar or N₂. In another embodiment, the spinel metaloxide may be a solid layer on the inorganic substrate layer 26, andcomprise 100 wt % spinel metal oxide. In one embodiment, a spinel metaloxide comprising nanostructures has some or all nanostructureschemically bonded and/or physically adsorbed to the inorganic substratelayer 26 and/or the light absorption layer 30. In another embodiment, amatrix material of the photoactive layer 28 may be chemically bondedand/or physically adsorbed to the inorganic substrate layer 26 and/orthe light absorption layer 30.

In one embodiment, the inorganic substrate layer 26 and the photoactivelayer 28 form an isotype junction. This means that the two layers aresemiconductors in direct contact and both comprise the same type ofmajority charge carriers. For instance, both layers may be “p-type” orhole-conducting, where the holes are the majority carriers and electronsare the minority carriers. Alternatively, both layers may be “n-type” orfree-electron conducting, where electrons are the majority carriers andthe holes are the minority carriers. The inorganic substrate layer 26and the photoactive layer 28 may have similar concentrations for aparticular majority carrier, or they may have different concentrationsfor a particular majority charge carrier. Alternatively, the inorganicsubstrate layer 26 and the photoactive layer 28 may have similarconcentrations but different motilities of a certain majority chargecarrier. In a preferred embodiment, both layers are “p-type,” orhole-conducting semiconductors.

The light absorption layer 30 of the photodiode comprises nanomaterialssuch as quantum dots, quantum rods, and/or quantum wires. The lightabsorption layer 30 may comprise 65-99 wt %, preferably 70-95 wt %, morepreferably 80-90 wt % nanomaterials, with the remaining compositioncomprising an inorganic or organic semiconductor matrix as mentionedpreviously, or a polymer matrix as described previously to encapsulatethe nanomaterial and restrict the movement of individual particles. Thisnon-nanomaterial composition may be chosen to modify an optical orelectronic property of the light absorption layer 30, such as a dye. Thedye may be coumarin, an organic laser dye, a porphyrin derivative, aninorganic complex of ruthenium, osmium, or iron, riboflavin, eosin, rosebengal, rhodamine B, cyanine, calconcarboxylic acid, or some other dye.Alternatively, the non-nanomaterial may not contribute significantly tothe optical or electronic properties. Similar to what was previouslymentioned for the spinel metal oxide, the light absorption layer 30 mayalso comprise air or an inert gas. One or more components of the lightabsorption layer 30 may be chemically bonded or physically adsorbed tothe photoactive layer 28.

In one embodiment, the light absorption layer 30 has a thickness of10-100 nm, preferably 15-80 nm, more preferably 20-70 nm, though in analternative embodiment, the light absorption layer 30 may have athickness less than 10 nm or greater than 100 nm. Preferably the lightabsorption layer 30 is able to absorb light of a wavelength 150-1500 nm,more preferably 200-1200 nm, even more preferably 400-1000 nm. Thisabsorption property may be a result of the quantum dots, quantum rods,and/or quantum wires having a band gap energy that corresponds to awavelength within or larger than that wavelength range. Preferably thenanostructure of the quantum dot, rod, or wire is able to confineconduction band electrons, valence band holes, or excitons (bound pairsof conduction band electrons and valence band holes) in all threespatial directions. This confinement may be due to electrostaticpotentials (such as those generated by external electrodes, doping,physical strain, or impurities), the presence of an interface betweentwo semiconductor materials (such as in core-shell or layerednanostructures) or at the interface between a semiconductor and anothermaterial. For example, a semiconductor may be decorated by organicligands or covered by a dielectric. This dielectric may be an oxide suchas PbO, a sulfite such as PbSO₃, a sulfate such as PbSO₄, or SiO₂. Inaddition, the confinement property may arise from the presence of thephotoactive layer 28. Due to this confinement, quantum dot, rod, or wirenanostructure exhibits in its absorption spectrum the effects of adiscrete quantized energy spectrum of an idealized zero-dimensionalsystem. The wave functions that correspond to this discrete energyspectrum are substantially spatially localized within the nanostructure,but may extend over many periods of the crystal lattice of the material.

As defined herein, quantum dots are nanoparticles having longest andshortest dimensions within 1-15 nm, where the ratio of the longest toshortest dimension is 1:1-1.5:1, preferably 1:1-1.2:1. Quantum dots mayhave a spherical or rounded shape, a cubic shape, or some other shape.As defined herein, quantum rods are nanoparticles having a shortestdimension of 1-15 nm and a longest dimension of 2-50 nm, where the ratioof the longest to shortest dimension is 1.5:1-5:1, preferably 2:1-4:1.The quantum rods may have a cylindrical shape, a rectangular shape, anellipsoidal shape, or may be some other elongated shape. As definedherein, quantum wires are nanoparticles having a shortest dimension of1-15 nm and a longest dimension of 50 nm-1 μm, where the ratio of thelongest to shortest dimension is 5:1-1,000:1, preferably 8:1-100:1. Inanother embodiment, the nanostructures of the light absorption layer 30may have other shapes, such as those listed previously for the spinelmetal oxide.

In one embodiment the nanomaterials of the light absorption layer 30comprise lead sulfide (PbS), lead selenide (PbSe), lead telluride(PbTe), cadmium selenide (CdSe), cadmium sulfide (CdS), and/or cadmiumtelluride (CdTe). In other embodiments the quantum dots, quantum rods,and/or quantum wires may comprise other materials such as cesium leadhalide perovskites (CsPbX₃, where X═Cl, Br, or I), indium arsenide(InAs), indium phosphide (InP), indium gallium arsenide (InGaAs),cadmium selenide sulfide (CdSeS), zinc sulfide (ZnS), silicon (Si), orsome other semiconductor material. The surface of the nanomaterials maybe passivated by physical adsorption or chemical attachment of ligands.These ligands may be thiol-terminated ligands such as benzenethiol,ethanethiol; carboxylate-terminated molecules such as oleic acid andformic acid; amine-terminated ligands such as pyridine, butylamine, oroctylamine; bidentate crosslinkers such as benzenedithiol,ethanedithiol, or butanedithiol. The ligands may include multidentatemolecules that have a backbone, certain side-groups and/or end-groupsthat bind to the nanoparticle surface, and other functional groups thatmay confer solubility in polar, nonpolar, and partially polar solvents.In another embodiment, the ligand may be an organophosphorous compoundsuch as trioctylphosphine oxide (TOPO). Alternatively, the surface ofthe nanostructures may have a dielectric, such as those mentionedpreviously. In one embodiment, the nanostructure can have a core-shellstructure with a semiconductor core, such as PbS. In some embodiments,the cores of adjacent nanostructures may be fused together to form acontinuous film of nanocrystal material to allow current to flow moreeasily while retaining nanoscale quantum effects.

In one embodiment the light absorption layer 30 may contain a mixture ofnanomaterials with one or more different properties of shape, size, orcomposition. For instance, a light absorption layer 30 may comprise 2-12nm, preferably 4-11 nm, more preferably 5-10 nm cubic PbS quantum dotsand 3-10 nm, preferably 4-9 nm, more preferably 5-8 nm hexagonal prismCdSe quantum dots at a mass ratio of 1:1-1:10, preferably 1:1-1:5, morepreferably 1:2-1:3. Alternatively, a light absorption layer 30 maycomprise PbSe in the form of quantum dots, rods, and wires having adistribution of shapes spanning from widths of 5 nm to lengths of 1 μm.In one embodiment, nanomaterials may be alloyed or comprise a core-shellstructure. For instance, a quantum dot may comprise a CdSe core of 3-6nm diameter surrounded by a ZnS shell layer with a 1-2 nm thickness.Preferably the optical properties of the light absorption layer 30 maybe adjusted by changes to its thickness or changes to the abovementionedproperties of the nanomaterial.

In one embodiment, the optical band gap of the photoactive layer 28 isgreater than the optical band gap of the light absorption layer 30,preferably by at least 0.2 eV, more preferably by at least 0.4 eV.However, in an alternative embodiment, the optical band gap of thephotoactive layer 28 is equal to or less than the optical band gap ofthe light absorption layer 30.

The top electrode 32 may comprise a conductive metal or metal alloy suchas those mentioned previously for the ohmic contact 24. In oneembodiment, the top electrode 32 is aluminum.

In one embodiment, the top electrode 32 does not completely cover thephotoactive layer 28. For instance, the top electrode 32 may exist as aplurality of circles with diameters of 0.5-3 mm, preferably 0.5-2 mm,more preferably 0.8-1.2 mm, and having a nearest neighbor spacing of0.5-10 mm, preferably 0.8-5 mm. The circles may be arranged in ahexagonal or square array, and may cover 5-50%, preferably 8-40%, morepreferably 10-20% of the surface of the photoactive layer 28.Alternatively, the top electrode 32 may comprise rectangles, squares, orsome other shape with widths similar to the previously mentioned circlediameters. In one embodiment, the circles may be electrically connectedto one another by a strip of conductive metal on the surface of thephotoactive layer 28. Alternatively, the circles may be electricallyconnected to one another by wires or other forms of conductive metalthat do not make contact with the surface of the photoactive layer 28.In another embodiment, the top electrode 32 may comprise interweavinglines as illustrated by the top electrode 32 in FIG. 2. The lines mayhave widths and spacings of 0.1-5 mm, preferably 0.2-2 mm, morepreferably 0.3-1 mm.

The top electrode 32 may have a layer thickness of 50 nm-5 μm,preferably 75 nm -1 μm, more preferably 100 nm-500 nm, and may be formedby evaporating or sputtering a metal onto the photoactive layer 28. Inan alternative embodiment, the top electrode 32 forms a contiguous layerand completely covers the photoactive layer 28. In this alternativeembodiment, the top electrode 32 may have an overall thickness orregions of different thicknesses that enable it to be transparent, andthe top electrode may comprise at least one of indium tin oxide (ITO),cadmium tin oxide, fluorine-doped tin oxide (FTO), aluminum-doped zincoxide (AZO), antimony-tin mixed oxide (ATO), a conductive polymer, anetwork of metal nanowire, a network of carbon nanowire, nanotube,nanosheet, nanorod, carbon nanotube, silver nanowire, or graphene.

Preferably the ohmic contact 24 and the top electrode 32 are each ableto electrically connect to a separate wire and/or charged surface. Theohmic contact 24 may form a cathode and the top electrode 32 may form ananode. As mentioned previously, the work function of the top electrode32 is greater than the work function of the ohmic contact 24, preferablyby at least 0.2 eV, more preferably by at least 0.5 eV. As used herein,the work function refers to the minimum energy needed to remove anelectron from a solid to a point in the vacuum immediately outside thesolid surface on an atomic scale. The work function is not acharacteristic of a bulk material, but rather a property of the surfaceof the material. In general, the work function tends to be smaller formetals with an open lattice, and larger for metals in which the atomsare closely packed. It is somewhat higher on dense crystal faces thanopen crystal faces, also depending on surface reconstructions for thegiven crystal face. The work function can also be determined by physicalfactors including, but not limited to, surface dipoles, doping, andelectric field effects. In an alternative embodiment, the work functionof the top electrode 32 may be less than or equal to the work functionof the ohmic contact 24.

In an alternative embodiment, a photodiode may be fabricated with amissing layer and yet still function as a photodiode or a rectifyingdiode. For instance, one layer selected from the light absorption layer30, the photoactive layer 28, or the inorganic substrate layer 26 may beomitted from the structure while retaining other layers. As each ofthese two layers may have semiconductor properties, a photodiode with amissing layer may still be able to form a P-N junction, or an isotypeP-P or N-N junction.

As mentioned previously, the top electrode 32 may be in contact but notcontinuous contact with the light absorption layer 30, as shown in FIG.2. In a related alternative embodiment, other layers of the photodiodemay be in contact, but not in continuous contact with an adjacent layer.For example, the ohmic contact 24 and the inorganic substrate layer 26may be in contact but not in continuous contact. Alternatively, thephotoactive layer 28 and the inorganic substrate layer 26 may be incontact but not in continuous contact. Alternatively, the lightabsorption layer 30 may be in contact with the photoactive layer 28 butnot in continuous contact. Where two layers are in contact without beingin continuous contact, one or both layers may be pattered with differentstructures, such as those mentioned previously for the light absorptionlayer 30. The voids where adjacent layers are not in contact may befilled with air, an inert gas, an insulating material, a conductivemetal as described previously, or a semiconductor (inorganic ororganic), or polymer material as described previously. The void may alsobe filled with a buffer layer material. In one embodiment, where layersare in contact but not in continuous contact, the voids may be patteredcorrals meant to segment regions of the photodiode or form separatecells.

In a related alternative embodiment, a photodiode may be fabricated withone or more additional buffer layers to block current leakage, to blocklight passage, or to provide some other functionality. The one or morebuffer layers may comprise materials such as a metal oxide (for example,tin oxide, indium oxide, calcium oxide, titanium oxide, zinc stannate,and/or zinc oxide), LiF, CsF, LiCoO₂, Cs₂CO₃, Al₂O₃, bathocuproine(BCP), copper phthalocyanine (CuPc), pentacene, pyronin B,pentadecafluorooctyl phenyl-C₆₀-butyrate (F-PCBM), C₆₀/LiF, ZnOnanorods/PCBM, ZnO/cross-linked fullerene derivative (C-PCBSD),polyethylene glycol (PEG), poly(dimethylsiloxane-block-methylmethacrylate) (PDMS-b-PMMA), polar polyfluorene (PF-EP), polyfluorenebearing lateral amino groups (PFN), polyfluorene bearing quaternaryammonium groups in the side chains (WPF-oxy-F), polyfluorene bearingquaternary ammonium groups in the side chains (WPF-6-oxy-F), fluorenealternating and random copolymer bearing cationic groups in the alkylside chains (PFNBr-DBT15), fluorene alternating and randomcopolymer-bearing cationic groups in the alkyl side chains (PFPNBr),polyethylene oxide (PEO), fullerene and derivatives thereof, a perylenederivative, a 2,7-dicyclohexyl benzo[lmn][3,8]phenanthroline derivative,a 1,4-diketo-3,6-dithienylpyrrolo[3,4-c]pyrrole (DPP) derivative, atetracyanoquinodimethane (TCNQ) derivative, indene-C₆₀ bisadduct([60]ICBA), indene-C₇₀ bisadduct ([70]ICBA), a poly(p-pyridyl vinylene)(PPyV) derivative, a 9,9′-bifluorenylidene (99BF) derivative, abenzothiadiazole (BT) derivative, [6,6]-phenyl C₆₁-butyric acid methylester (PCBM), [6,6]-phenyl C₆₁-butyric acid methyl ester (PC70BM),[6,6]-(4-fluoro-phenyl)-C₆₁-butyric acid methyl ester (FPCBM), carbon 60(C₆₀), carbon 70 (C₇₀), carbon nanotube (CNT), or combinations thereof.These additional buffer layers may also comprise one or more inorganicor organic semiconductor matrix material or polymer matrix material asmentioned previously. One or more buffer layers may form chemical bondsto one or more adjacent surfaces, and/or may be physically adsorbed,though some buffer layers may sit in direct contact without adsorptionor chemical bonding. The one or more buffer layers may be any thicknessas previously discussed for the other components of the photodiode, or asmaller thickness, and may have a constant or varying thicknessthroughout its volume. Additionally, one or more buffer layers may notbe in continuous contact with adjacent layers. In another relatedalternative embodiment, the top electrode 32 and optionally, the lightabsorption layer 30, may be coated with a transparent layer to protectthe photodiode but allow passage of light to the light absorption layer30.

In one embodiment, the photodiode has a barrier height of 0.5-1.25 eV,preferably 0.6-1.1 eV, more preferably 0.7-1.0 eV. As used herein, thebarrier height refers to a potential energy barrier for electrons formedat a junction between a metal and a semiconductor. This may also becalled a Schottky barrier height and may be denoted by the symbol Φ_(B).This energy barrier is rectifying, meaning that the junction may onlyconduct current in one direction. However, in other embodiments, thephotodiode may have a lower or negligible barrier height, where themetal and semiconductor junction allows current flow in both directions.

In one embodiment, the photodiode has a photoresponsivity of 0.10-0.40A/W, preferably 0.20-0.40 A/W, more preferably 0.25-0.35 A/W. In oneembodiment, these photoresponsivity values arise at a reverse biasvoltage of 3-8 V, preferably 4-7 V, and under an illumination powerdensity of 100 mW/cm². As used herein, the photoresponsivity is a ratioof the photodiode's generated photocurrent to the incident radiationpower. FIG. 5 shows a plot of an exemplary photodiode'sphotoresponsivity to bias voltage. In one embodiment, the photodiode'sdensity of interface states relates to its photoresponsivity. Forexample, increasing the density of interface states from 1×10¹¹ eV⁻¹ cm²to 1×10¹³ eV⁻¹ cm⁻² may cause the photoresponsivity to increase from 0.2A/W to 0.4 A/W. As defined here, the density of interface states refersto the density of energy levels at the surface between a semiconductorand a conductor. These interface states may also be called interfacetraps, and arise as a result of the unpaired valence electrons at theface of the semiconductor. These unpaired valence electrons mayinterfere with passing current. The density of interface states and thephotoresponsivity may both be influenced by the frequency and directionof a bias current applied to the photodiode. In one embodiment, theinterface states can follow an alternating bias current at lowfrequencies and can contribute to the total capacitance of thephotodiode. However, at high frequencies, the interface states cannotfollow the current and thus do not contribute significantly to thecapacitance of the diode. The density of interface states may alsodepend on the orientation of the semiconductor lattice.

The ideality factor, n, of the photodiode may be 1-6, preferably 2-5.The ideality factor is a dimensionless quantity that can be derived fromthe slope of the linear part of the forward bias semi-log I vs. V plotthrough the relation:

${n = {\frac{q}{KT}\frac{d\; V}{d\;{\ln(I)}}}},$where q is the electronic charge, V is the applied voltage, k isBoltzmann's constant, T is the temperature in Kelvin, and I is thecurrent.

In one embodiment, the photodiode has a photosensitivity of 6000-7500,preferably 6500-7000 at a bias of 5.0-8.0 V, preferably 6.0-7.5 V.Preferably the bias of 5.0-8.0 V is applied as a reverse bias, with thepositive voltage applied to the cathode (ohmic contact 24) and thenegative voltage applied to the anode (top electrode 32). The value ofphotosensitivity used here is the ratio of the photodiode's photocurrentto dark current, and in some cases, the photosensitivity may be calledthe photocurrent gain. FIG. 6 shows a plot of an exemplary photodiode'sphotosensitivity over a range of forward (positive) and reverse(negative) bias voltages and under an illumination power density of 100mW/cm². FIG. 4 shows a photocurrent vs. bias voltage plot of anexemplary photodiode under different illumination power densities. Anincreasing power density increases the photocurrent when a reverse biasvoltage (negative voltage value) is applied. With forward bias voltages,the illumination power density produces a negligible difference on theamount of photocurrent. This behavior at forward and reverse biasvoltages is typical for a photodiode.

According to a second aspect, the present disclosure relates to a methodfor forming the photodiode of the first aspect. These steps involvedepositing the ohmic contact 24 onto the inorganic substrate layer 26;spin or drop coating the spinel metal oxide onto the inorganic substratelayer 26, to form the photoactive layer 28; spin or drop coating quantumdots, quantum rods, or quantum wires onto the photoactive layer 28,thereby forming the light absorption layer 30; and depositing the topelectrode 32 onto the light absorption layer 30. Each layer may be addedor deposited to the layer thicknesses such as those mentioned previouslyfor the photodiode. However, in alternative embodiments, one or morelayers may have a thickness that is greater or less than that previouslymentioned. In some embodiments, a layer deposition step may be repeatedin order to increase its thickness.

Fabrication steps are outlined in the flowchart 10 of FIG. 1. Here, aninorganic substrate layer 26 is obtained. This inorganic substrate layer26 is a semiconductor, and may be in the form of a silicon wafer. In apreferred embodiment, the semiconductor is a p-type siliconsemiconductor, though in other embodiments it may be n-type or anon-silicon semiconductor such as those listed previously. Thisinorganic substrate layer 26 may have a thickness and other propertiessuch as those listed previously, and may be prepared for fabrication 12by cleaning in a chemical bath and/or sonication. For example, thechemical bath may be one or more organic solvents such as acetone,methanol, ethanol, hexane, or isopropanol. The inorganic substrate layer26 may be rinsed with the organic solvents or submerged and soaked for1-18 hours, preferably 2-5 hours. Alternatively, the inorganic substratelayer 26 may be submerged and sonicated in the chemical bath for 1-30min, preferably 5-10 min. Preferably, after cleaning with an organicsolvent, the inorganic substrate layer 26 may be rinsed with distilledor deionized water. Alternatively, the inorganic substrate layer 26 maybe cleaned by sonicating in distilled or deionized water and withoutusing an organic solvent. Following the cleaning with organic solvent orwater, the inorganic substrate layer 26 may be dried under a stream ofAr or N₂ gas, or in a desiccator.

The ohmic contact 24 may then be deposited 14 onto one surface of theinorganic substrate layer 26. This deposition may be a metal depositionand accomplished through thermal evaporation of the metal, for example,at a pressure of 10⁻⁴-10⁻⁸ Torr, preferably 10⁻⁴-10⁻⁶ Torr. In anotherembodiment, the metal may be deposited 14 through metal sputtering,e-beam evaporation, or pulsed laser deposition. In another embodiment,the metal may be pre-formed as a thin plate or foil, and may bedeposited 14 by placing it onto the surface of the inorganic substratelayer 26. The metal may be any of those listed previously for the ohmiccontact 24.

The spinel oxide may then be spin or drop coated 16 onto a secondsurface of the inorganic substrate layer 26 at a spinning rate of1,000-8,000 RPM, preferably 2,000-6,000 RPM. Alternatively, the spineloxide may be deposited by an ink-jet printing process, Langmuir-Blodgettfilm deposition, electrokinetic spray, a dip coating process, ornano-imprint. Here the spinel oxide may be suspended in a solution at aconcentration of 0.01-60 wt %, preferably 0.1-65 wt %, more preferably1-50 wt %. The solvent may be ethanolamine, toluene, chloroform,pyridine, isopropanol, butanol, acetone, ethanol, ethylene glycol,and/or water. In one embodiment, metal nitrate salts may be used withethanol to form the spinel oxide. The metal nitrate salts may have aconcentration of 0.1 M-2 M, preferably 0.2-1 M, more preferably 0.3-0.8M. In another embodiment, metal chloride salts may be used withethanolamine at a similar concentration range to form the spinel oxide.The spinel oxides formed may be in the form of different nanostructuredmaterials as mentioned previously.

The layer thickness may be controlled by the spinning rate, the volumeof solution added, and the number of layers deposited. The spinel oxidelayer may also be called the photoactive layer 28. In one embodiment,the inorganic substrate layer 26 may be dried after one or more spin ordrop coatings by heating in an oven or on a hot plate at 150-250° C. for4-15 minutes to evaporate the solvent. Alternatively, the inorganicsubstrate layer 26 may be left to dry in a desiccator at roomtemperature. Then, a solution of quantum dots, quantum rods, and/orquantum wires may be deposited onto the spinel oxide layer by spincoating, drop coating, dip coating, ink-jet printing, Langmuir-Blodgettfilm deposition, electrokinetic spray, or nano-imprint. The quantumdots, quantum rods, and/or quantum wires may be suspended in a solventsuch as those mentioned previously, at a concentration of 0.01-60 wt %,preferably 0.1-65 wt %, more preferably 1-50 wt %. In one embodiment,quantum dots may be used at a concentration of 0.1-2.0 M, preferably0.2-1.0 M, more preferably 0.3-0. M in ethanol or methanol.

The layer of quantum dots, rods, and/or wires forms the light absorptionlayer 30 of the photodiode.

The inorganic substrate layer 26 having the ohmic contact 24 and thephotoactive layer 28 may undergo thermal annealing 18. For this, theinorganic substrate layer 26 may be heated at 400-800° C., preferably500-750° C., more preferably 600-725° C. for 30 min -3 h, preferably 45min-1.5 h. In one embodiment, the inorganic substrate layer 26 havingthe ohmic contact 24 and the photoactive layer 28 may be heated at alower temperature before and/or after the annealing. This heating may beat 100-200° C., preferably 110-180° C., more preferably 130-170° C. inair for 4-30 min, preferably 5-20 min, more preferably 8-15 min. In analternative embodiment, the inorganic substrate layer 26 is notannealed.

In one embodiment, the light absorption layer 30 may be deposited afterthe thermal annealing, and then undergo a second annealing step byheating at 150-400° C., preferably 160-300° C., more preferably 180-250°C. for 4-30 min, preferably 5-20 min, more preferably 8-15 min. In analternative embodiment, the thermal annealing step may come after thephotoactive layer 28 and the light absorption layer 30 have beendeposited.

Next, a metal may be deposited 20 onto the light absorption layer 30 toform the top electrode 32. This creates the photodiode. Preferably themetal is deposited 20 by evaporation through a patterned mask in orderto not completely cover the surface of the light absorption layer 30.The metal may be deposited 20 as patterns as mentioned previously. In apreferred embodiment, the metal may be evaporated through a shadow maskhaving an array of 1 mm diameter circles. In one embodiment the metal isdeposited without a patterned mask and is instead pattered afterwards bychemical etching. In another embodiment, the metal may be pre-formed asa thin plate or foil, and may be placed onto the light absorption layer30. In this embodiment, the metal may be cut or etched into a patternbefore being placed, or the metal may be placed and then cut or etchedinto a pattern.

The photodiode may be housed in a casing to connect electrical leads tothe top electrode 32 or ohmic contact 24 and/or protect the photodiodesurface. This casing may comprise an insulated metal, of such metals asthose listed previously, a polymeric material such as polylactic acid(PLA), poly(lactic-co-glycolic acid) (PLGA), polyethylene terephthalate(PET), acrylonitrile butadiene styrene (ABS), and/orpolytetrafluoroethylene (PTFE), or some other non-metal, such as glassor ceramic. Preferably the casing has an opening or transparent windowto allow the passage of incident light. The photodiode may then becharacterized 22 for its optoelectric properties, including, but notlimited to photoresponsivity, photosensitivity, resistance, capacitance,response time, and barrier height. This type of testing may be completedusing instrumentation such as a Kiethley 4200 semiconductorcharacterization system, or some other parameter analyzer. Thephotodiode may be tested with illumination from one or more wavelengthsin the range of 150-1,500 nm, preferably 200-1,000 nm, and irradiatingthe photodiode with a power density of 1-1,000 mW/cm², preferably 10-500mW/cm², more preferably 20-200 mW/cm². The irradiation may be generatedfrom a flame, a lantern, a gas discharge lamp, an incandescent bulb, alaser, a fluorescent lamp, an electric arc, a light emitting diode(LED), a cathode ray tube, solar light 34, and/or some other source oflight, and may be manipulated with filters, shutters, reflectors,diaphragms, optical fibers, or other optics. A light power meter may beused to measure the intensity and optionally the wavelength of theirradiated light.

According to a third aspect, the present disclosure relates to a methodof generating an electronic current using the photodiode of the firstaspect. This method involves irradiating the photodiode of the firstaspect with a light source having a wavelength of 150-1500 nm. In oneembodiment, the light may be of a wavelength, power density, and sourceas mentioned previously. In one embodiment, the light absorption layer30 absorbs light of a certain energy and fluoresces or phosphoresceslight of a lower energy, which may go on to interact with thephotoactive layer 28. A forward or reverse bias voltage of −10 to 10 V,preferably −7 to 7 V, more preferably −6 to 6 V may be applied to thephotodiode.

In another embodiment, the light absorption layer 30 may be designed asa filter, where it to absorbs or reflects light of certain propertieswhile allowing other light to pass through to the spinel oxidesemiconductor. These properties may be based on the wavelength,polarization, and/or incidence angle of the light.

In some embodiments, a light absorption layer 30 may be designed tomaximize certain wavelengths of light arriving to the spinel oxidesemiconductor from a broad wavelength light source. For example, a lightabsorption layer 30 may absorb solar light 34 having wavelengths in therange 250-450 nm, while transmitting or allowing light of 550 nmwavelength and higher to pass through. The light absorption layer 30 mayphosphoresce or fluoresce the absorbed energy as light with wavelengthsabove 550 nm, which light then irradiates the spinel oxide semiconductorto produce electron hole pairs. Thus, the light absorption layer 30 maybe used to change the properties of the light received by the spineloxide semiconductor.

In one embodiment, the light absorption layer 30 absorbs light andtransfers energy to the photoactive layer 28 using a non-radiativeprocess. For example, the light absorption layer 30 may produce ahole-electron pair which transfers the energy, or the light energy maybe absorbed and transferred by Förster resonance energy transfer (FRET),surface energy transfer (SET), Dexter energy transfer, or some otherprocess.

In one embodiment, the top electrode 32 may absorb a photon and emit anelectron through a photoelectric effect. The electron may then interactwith the light absorption layer 30 or photoactive layer 28.

In one embodiment, light absorbed by the light absorption layer 30, thephotoactive layer 28, or the inorganic substrate layer 26 may produceone or more free electron hole pairs in the material. The free electronand the hole may recombine, or may drift through the material and crossinto different layers. Electrons or holes reaching the top electrode 32and/or ohmic contact 24 may produce a measurable change in current.

According to a fourth aspect, the present disclosure relates to anelectronic device comprising the photodiode of the first aspect. In apreferred embodiment, the photodiode may be used as a photodetector. Areverse bias voltage may be applied with a positive voltage at the ohmiccontact 24 (cathode) and a negative voltage at the top electrode 32(anode). Light transmitted to the photoactive layer 28 or other layersmay be detected by an increased current flowing through thephotodetector. Alternatively, without light illumination, the photodiodemay be used as a rectifying diode, where current having a forward biasvoltage may flow through the diode with less resistance than currenthaving a reverse bias voltage.

In another embodiment, the photodiode may be used as a photovoltaicdevice, with the purpose of generating electric energy from irradiatedlight. In this embodiment, the photodiode may not have a reverse orforward bias applied to it, and may be designed with a slower responsetime and a larger exposed area than a photodiode designed as aphotodetector.

In another embodiment, a photodetector array is envisioned includingindividually selectable anode lines and individually selectable cathodelines running perpendicular with the photoactive layer 28 describedherein disposed between them. In this manner, each intersection of oneof the anode lines and one of the cathode lines forms an individuallyselectable photodetector. These photodetectors offer applications infiber optic communications, safety and security, process control,environmental sensing, astronomy, and defense.

In another embodiment, the photodiode described herein can have arolled-up or spiral structure. In a related embodiment, one or morephotodiodes may be incorporated into flexible electronic devices.Alternatively, a rolled-up or spiral structure is envisioned to functionas an ionizing radiation detector with the ability to detect X-rays orgamma rays, or may function as a particle detector with the ability todetect neutrons and other subatomic particles. In another embodiment,one or more photodiodes may be incorporated into a touch-sensitivescreen, in order to create a photosensitive device.

In another embodiment, the photodiode is envisioned to have applicationsin a number of different non-limiting circuits. In cameras this includeslight meters, automatic shutter control, auto-focus, and photographicflash control. In medicine, this includes CAT scanners, X-ray detection,pulse oximeters, and blood particle analyzers. In communications, thisincludes fiber optic links, optical remote controls, and opticalcommunications. In safety, this includes smoke detectors, flamemonitors, intruder alert security systems, and security inspectionsystems. In industrial settings, this includes bar code scanners, lightpens, brightness controls, encoders, positions sensors, surveyinginstruments, and copiers. In the automotive industry, this includesheadlight dimmers, twilight detectors, and climate control-sunlightdetectors.

The examples below are intended to further illustrate the photodiode andprovide protocols for preparing and characterizing the photodiode, anduses thereof, and are not intended to limit the scope of the claims.

Example 1

Fabrication Process

In one embodiment of the invention, a high photoresponsivity isotypephotodiode is provided. A diode based on an isotype junction wasfabricated on a p-type spinel oxide semiconductor and a p-typeconventional silicon wafer. The diode has the structure: Al/quantumdots/spinel oxide layer/p-Si/Al.

The isotype junction photodiode was fabricated on p-type silicon, thep-type silicon having a 400 μm thickness, a resistivity of 1-10 Ω·cm,and a (100) orientation. The p-type silicon substrate is doped to have acharge carrier concentration of 10¹⁵ to 10¹⁶ cm⁻³. The p-type siliconsubstrate alone was cleaned by chemical baths, followed by ultrasonictreatment for 5 minutes.

Al metal was coated to a 100 nm thickness on the back side of the p-typesilicon wafer by thermal evaporation or a sputtering method in a highvacuum chamber with a pressure of 10⁻⁵ Torr. Next, the Al-coated waferwas annealed at a eutectic temperature of 570° C. for 5 hours innitrogen to obtain the ohmic contact.

The spinel oxide layer comprises a metal oxide with the formulaA²⁺(B³⁺)₂(O²⁻)₄, such as AFe₂O₄, where “A” is Zn, Cu, Co, and/or Mn.Each of these spinel oxides were synthesized and used in a photodiode.Each spinel oxide was deposited on the p-type silicon layer by a spincoating or drop casting method to a thickness of 50-100 nm. The spineloxide layer semiconductor absorbs light in the spectral region of 350 nmto 700 nm. The absorption of the photoactive layer 28 may be tuned usinga light absorption layer 30 comprising quantum dots, quantum rods,and/or quantum wires. The light absorption layer 30 used here is made ofquantum dots such as cadmium sulfur (CdS), cadmium selenium (CdSe),cadmium telluride (CdTe), lead sulfide (PbS), lead selenium (PbSe), andlead telluride (PbTe).

The quantum dots were synthesized from precursor salts. For example, CdSquantum dots were prepared by mixing 0.5 M Cd(NO₃)₂ in ethanol (cadmiumcationic precursor) with 0.5 M Na₂S in water (sulfur anionic precursor).CdSe and other quantum dots were prepared similarly with differentprecursor salts. To deposit the quantum dots, the spinel oxide filmswere dipped into this solution of quantum dots for 5 min, rinsed withethanol, dried for 10 min, and allowed to cool to room temperature. Thisdipping procedure may be repeated three or more times to increase thequantum dot layer thickness. Then, the films were annealed at 300° C.for 10 min.

Finally, the top Al electrode was evaporated to a 100 nm thicknessthrough a shadow mask with 1 mm diameter circles. The top electrode Alforms a Schottky contact with the spinel oxide layer. The photodiode hasa contact area of 3.14×10⁻² cm², formed by a dot with a 2 mm diameter.

The electrical and photoresponse properties of the photodiodes in darkand under solar illumination from a 150 W solar simulator were measuredusing a Keithley 4200 semiconductor characterization system. Theillumination intensity was changed using a variable power supply andoptical meter. The photoconductive gain (photosensitivity) was measuredas 6500-7000 at 7 V reverse bias under an illumination power density of100 mW/cm² (FIG. 6).

The invention claimed is:
 1. A photodiode, comprising: an ohmic contacthaving a first work function; an inorganic substrate layer in continuouscontact with the ohmic contact; a photoactive layer in continuouscontact with the inorganic substrate layer; a light absorption layer incontinuous contact with the photoactive layer; and a top electrode incontact with the light absorption layer, the top electrode having asecond work function; wherein the inorganic substrate layer comprises asemiconductor; wherein the light absorption layer is made of anabsorption composition comprising 70-95 wt % of quantum dots of at leastone material selected from the group consisting of lead sulfide (PbS),lead selenide (PbSe), lead telluride (PbTe), cadmium selenide (CdSe),cadmium sulfide (CdS), and cadmium telluride (CdTe), with the remainingportion of the absorption composition a polymer matrix; wherein thephotoactive layer consists of ZnFe₂O₄ nanowires in N₂, the ZnFe₂O₄nanowires present at 80-90 vol % relative to a total volume of thephotoactive layer; wherein the ZnFe₂O₄ nanowires have widths of 35-45 nmand lengths of 170-350 nm; wherein all ZnFe₂O₄ nanowires are physicallyadsorbed to the inorganic substrate layer and to the light absorptionlayer; wherein the inorganic substrate layer and the photoactive layerare both p-type semiconductors forming an isotype junction between eachother; and wherein the second work function is higher than the firstwork function.
 2. The photodiode of claim 1, wherein the inorganicsubstrate layer has a thickness of 200-600 μm.
 3. The photodiode ofclaim 1, wherein the photoactive layer has a thickness of 20-250 nm. 4.The photodiode of claim 1, wherein the light absorption layer has athickness of 10-100 nm.
 5. The photodiode of claim 1, wherein the topelectrode is aluminum.
 6. The photodiode of claim 1, wherein theinorganic substrate layer has a resistivity of 1-10 Ω·cm.
 7. Thephotodiode of claim 1, which has a barrier height of 0.5-1.25 eV.
 8. Thephotodiode of claim 1, which has a photoresponsivity of 0.10-0.40 A/W.9. The photodiode of claim 1, which has a photosensitivity defined asthe ratio of illuminated current to dark current of 6000-7500 at a biasof 5.0-8.0 V.